Tzu-Yun Huanga,
Yen-Jui Chena,
Chi-Yung Laib and
Yang-Wei Lin*a
aDepartment of Chemistry, National Changhua University of Education, Changhua, Taiwan, Republic of China. E-mail: linywjerry@cc.ncue.ed.tw
bGraduate Institute of Biotechnology, National Changhua University of Education, Changhua, Taiwan, Republic of China
First published on 8th May 2015
This novel Ag/Ag3PO4 nanostructure-sensitized BiPO4 (Ag/Ag3PO4/BiPO4) photocatalyst was synthesized using hydrothermal and impregnation processes. Powder X-ray diffraction, UV-Vis diffuse reflectance spectroscopy, Raman spectroscopy, IR spectroscopy, X-ray photoelectron spectroscopy, transmission electron microscopy, and scanning electron microscopy were used to characterize the as-prepared products. The optical properties and morphology of BiPO4 exhibited drastic changes and were dependent on the AgNO3 concentration. Regarding methylene blue (MB), rhodamine B, and methyl orange degradation under solar irradiation (95% degradation within 5 min), 15% Ag/Ag3PO4/BiPO4 exhibited considerably higher photocatalytic activity than BiPO4 and P25. After five cycles, Ag/Ag3PO4/BiPO4 exhibited no apparent loss of activity, confirming its stability despite recycling. The practicality of this Ag/Ag3PO4/BiPO4 was validated according to its ability to degrade MB in seawater, pond water, and industrial wastewater samples, which also demonstrated the advantages of its high photocatalytic activity. Moreover, 15% Ag/Ag3PO4/BiPO4 also showed sunlight-induced photocatalytic disinfection activity toward E. coli cells. The enhanced photocatalytic activity and improved stability of Ag/Ag3PO4/BiPO4 could be attributed to the strong visible light absorption by Ag/Ag3PO4 nanostructures, a low electron–hole recombination rate, and the highly efficient separation of photogenerated electron–hole pairs throughout Ag3PO4/BiPO4 heterostructures. Moreover, holes were the main reactive species.
Some novel materials, such as Bi- and V-based photocatalysts, have been synthesized in 2014 for finding materials with superior photocatalytic activity.5–9 Among them, BiPO4 has unique catalytic applications. Many systematic studies have analyzed the morphology-dependent photocatalytic activity, recyclability, and practicability of these catalysts.10,11 The high photocatalytic activity of BiPO4 was primarily attributed to the high energy of the valence band and high separation efficiency of electron–hole pairs.12,13 However, poor solar efficiency hindered the applicability of BiPO4. Therefore, developing photocatalysts that have high reactivity under visible light irradiation is crucial for overcoming the drawbacks of BiPO4. Recently, Ag3PO4 was found to demonstrate high performance in the photodecomposition of organic dyes in wastewater under visible light illumination.14,15 However, Ag3PO4 is not stable during the photocatalytic process because of photocorrosion, meaning that in the absence of an electron acceptor, the photogenerated electron decomposes Ag3PO4 on photoillumination.16–18 More recently, Ag3PO4/BiPO4-based heterostructures were prepared as a modification of Ag3PO4.19–21 For example, a BiPO4@Ag3PO4 core/shell heterojunction photocatalyst was synthesized using a facile hydrothermal process, followed by the ion-exchange method.19 The results showed that RhB was almost completely degraded in 60 min under visible light irradiation and in 40 min under solar irradiation. The BiPO4@Ag3PO4 core/shell heterojunction photocatalyst exhibited enhanced photocatalytic activity against RhB, which is attributed to the effective charge separation by the core/shell heterojuction between Ag3PO4 and BiPO4. One-step synthesis of a Ag/Ag3PO4/BiPO4 double-heterostructured photocatalyst was demonstrated by the Lv group.20 Higher photocatalytic activity and stability for the photodegradation of organic compounds (rhodamine B, RhB) were observed under visible light (98% RhB degradation, 60 min) because of both the formation of an effective heterostructure and the Schottky barrier effect. These two aspects contributed to the charge transfer between the metal and semiconductor and the separation of photogenerated electron–hole pairs; however, this research lacked the experimental evidence to prove these two suggestions. Ag3PO4/BiPO4 was synthesized using the co-precipitation hydrothermal method.21 The higher photocatalytic activity of Ag3PO4/BiPO4 (97% methyl orange (MO) degradation, 30 min) could be mainly attributable to strong visible light absorption and a high separation efficiency of electron–hole pairs. However, the stability study was not addressed. Notably, few photocatalytic results have demonstrated the practicability of the aforementioned Ag3PO4/BiPO4 photocatalysts.
This paper presents a systematic study of Ag/Ag3PO4/BiPO4 synthesis under hydrothermal conditions at 180 °C for 24 h and then calcination at 500 °C for 6 h. The photocatalytic activity, recyclability, and practicability of the synthesized Ag/Ag3PO4/BiPO4 were evaluated according to its ability to degrade methylene blue (MB), RhB, and MO in various water samples under visible light (λ > 420 nm) and solar irradiation. The mechanism of the photocatalytic degradation of organic pollutants by Ag/Ag3PO4/BiPO4 was also investigated.
Ag/Ag3PO4 samples were synthesized using a precipitation–hydrothermal process. The typical preparation was as follows: AgNO3 (1.25 mmol) and Na3PO4 (2.5 mmol) were placed in a beaker. Deionized water (46 mL) and HNO3 (4 M, 1 mL) were added to the beaker, and the mixture was magnetically stirred to form a homogeneous solution at room temperature. After 1 min, the yellow precipitate was transferred to a Teflon-lined stainless steel autoclave and maintained at 180 °C for 24 h. Yellow Ag/Ag3PO4 powders were obtained through centrifugation, washed three times with deionized water and ethanol, and then dried in a desiccator at 55 °C for 12 h.
The experimental procedure followed for examining holes and hydroxyl radical species was similar to that for the photocatalytic activity experiment.22 Various quantities of scavengers were introduced into the MB solution prior to the addition of the catalyst. In addition, a photoluminescence (PL) technique, with coumarin (1 mM) as a probe molecule, was used to investigate the formation of hydroxyl radicals on the surface of the photocatalysts (BiPO4 and 15% Ag/Ag3PO4/BiPO4) illuminated by visible light irradiation for 15 min.22
Fig. 1(b) shows the UV-DRS spectra of Ag/Ag3PO4, Ag/Ag3PO4/BiPO4, and BiPO4. Clearly, yellow Ag/Ag3PO4 possessed strong visible light absorption ability, whereas white BiPO4 possessed UV light absorption ability. Ag/Ag3PO4/BiPO4 exhibited absorption properties that were a mixture of those of Ag/Ag3PO4 and BiPO4. For semiconductor materials, the square of the absorption coefficient was linearly correlated with the energy for direct optical transitions in the absorption edge region, whereas the square root of the absorption coefficient was linearly correlated with the energy for indirect transitions. Data plots of the square root of the absorption coefficient versus the energy in the absorption edge region are shown in the inset of Fig. 1(b); the plots are approximately linear. These results suggested that the absorption edges of the three materials were because of indirect transitions; thus, the bandgap energies of the samples were estimated from the plots using the intercept of the tangent to the x-axis. The estimated bandgaps of as-synthesized Ag/Ag3PO4, Ag/Ag3PO4/BiPO4, and BiPO4 were approximately 2.08, 2.05, and 4.08 eV, respectively (inset of Fig. 1(b)). These results clearly confirm that the electronic structures of the as-synthesized materials differ. The variation in the bandgap may be due to different degrees of delocalization and mobility of the photoinduced electron–hole pairs, which may have also resulted in different photocatalytic efficiencies.
The structures of Ag/Ag3PO4, Ag/Ag3PO4/BiPO4, and BiPO4 were further characterized using Raman spectroscopy in the 100–1200 cm−1 region (Fig. S2A†). Notably, the Raman bands we observed in these spectra were consistent with literature data.25 For Ag/Ag3PO4/BiPO4 and BiPO4, the peaks between 100 and 300 cm−1 may be assigned to the symmetric bending vibration of the Bi–O bonds. One of the strong features of Raman spectroscopy is that bands below 400 cm−1 are readily observed. Thus, the intense bands attributable to M–O bond vibrations could be observed. However, Ag/Ag3PO4 exhibited no peaks in this region. For Ag/Ag3PO4/BiPO4 and BiPO4, the Raman bands between 460 and 600 cm−1 in the spectra in Fig. S2† were attributed to the v4 bending modes of the PO4 units, and those between 380 and 460 cm−1 were attributed to the v2 bending modes of the PO4 units. Ag/Ag3PO4 exhibited weak peaks corresponding to v2 and v4 bending vibrations of the PO43− moiety at 408 and 552 cm−1, respectively. The two intense bands between 960 and 1100 cm−1 were ascribed to the v1 symmetric and v3 antisymmetric stretching modes of the PO4 tetrahedron in case of Ag/Ag3PO4/BiPO4 and BiPO4, respectively. Ag/Ag3PO4 exhibited an intense peak at 908 cm−1, which was attributed to the symmetric stretching mode of the PO43− moiety under cubic symmetry. A similar peak was also observed in case of Ag/Ag3PO4/BiPO4, indicating the presence of the Ag3PO4 structure.
FTIR spectroscopy was also used to investigate the structures of the catalysts (Fig. S2B†). There are four asymmetric stretching (v3) vibrations of P–O bond resulting from the distortion of tetrahedral phosphate groups in monoclinic BiPO4. These bands are seen at 1070, 1010, 956, and 925 cm−1 in the as prepared BiPO4. The asymmetric bending (v4) vibrations of PO4 group appeared between 500 to 600 cm−1. These bands appeared at 596, 566, 555, and 528 cm−1, respectively. In the case of as-prepared Ag/Ag3PO4/BiPO4, the different relative intensities and wavenumber shifts of the v3 and v4 vibration indicate that a slight change in the structure of the PO4 tetrahedron.25
To further investigate the chemical and bonding environment of Ag/Ag3PO4/BiPO4 heterostructures, an XPS analysis was performed; the results are shown in Fig. S3,† where the C 1s peak at 285 eV serves as a calibration standard. In this figure, peaks from Bi, P, O, and Ag could be observed, thus proving the chemical composition of the heterostructures. Both the Bi and Ag bands exhibited distinct doublets because of spin–orbit coupling. The peaks at 159.8 and 164.8 eV were due to Bi4f7/2 and Bi4f5/2 levels in BiPO4, respectively. The peaks at 442.8 and 465.8 eV corresponded to Bi3d5/2 and Bi3d3/2 levels in BiPO4, respectively. The peak at 132.8 eV corresponded to P5+ in the PO43− of BiPO4, while those at 367.8 eV and 373.8 eV corresponded to Ag3d5/2 and Ag3d3/2, respectively. According to literature,19,26 the peak shift (6 eV) between Ag3d5/2 and Ag3d3/2 is in agreement on that of bulk Ag (Ag3d5/2, 368.2 eV; Ag3d3/2, 374.2 eV), indicating the appearance of zero-valent Ag in the Ag/Ag3PO4/BiPO4 heterostructure.19,26
Fig. 2 displays typical SEM and TEM images of BiPO4 and Ag/Ag3PO4/BiPO4 products prepared with an increasing Ag content (mass ratios of 3%, 15%, and 30%). Marked differences in the morphology and size of the as-prepared products can be clearly seen in these images. The BiPO4 comprises rod-like nanostructures (Fig. 2). The morphology and size of BiPO4 particles were further examined using TEM. The particles had diameters of 180.9 ± 49.3 nm and lengths of 2169.4 ± 257.0 nm. In a typical process for synthesis of BiPO4, Bi(NO3)3·5H2O and Na3PO4 was mixed with Milli-Q water in the presence of 4 M of HNO3. The mixture was stirred gently at room temperature for 1 min, at which time the white precipitate was formed, indicating the formation of small BiPO4 NPs. Then the white precipitate was transferred to a Teflon-lined stainless steel autoclave and maintained at 180 °C for 24 h. In the hydrothermal process, the primary particles may aggregate in an oriented fashion, resulting in the formation of a larger single crystal, or they may randomly aggregate and reorient.10 However, this aggregation-growth mechanism provides a route for the incorporation of defects; numerous cracks were observed on the surface in the HR-TEM image (Fig. 2(a)). In the HRTEM image of BiPO4, majority of the particles appeared to be composed of many primary building block particles ranging in size from less than 5 to 10 nm. It is thus assumed in BiPO4 rod-like structures that the primary particles aggregated in an oriented fashion, producing assemblies of oriented nanoparticles that subsequently underwent further growth.
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Fig. 2 Scanning electron microscopy (SEM), transmission electron microscopy (TEM), and HR-TEM images of (a) BiPO4, (b) 3% Ag/Ag3PO4/BiPO4, (c) 15% Ag/Ag3PO4/BiPO4, and (d) 30% Ag/Ag3PO4/BiPO4. |
Ag/Ag3PO4/BiPO4, which was impregnated with 3% Ag+, comprises irregular rod-like nanostructures with diameters of 195.6 ± 70.0 nm and lengths of 1625.7 ± 195.3 nm. As the BiPO4 reacted with water, the hydroxyl groups are generated on the surface of BiPO4 and produced chemical bonding with Ag+ ions.19 Through ion exchange process, Ag3PO4 particles would be formed on the cracks of BiPO4 surface, as a result short and irregular rod-like heterojunction nanostructures were produced (HR-TEM image in Fig. 2(b)). When the Ag+ content was increased to 15%, short rod-like Ag/Ag3PO4/BiPO4 particles with diameters of 171.7 ± 62.1 nm and lengths of 1252.6 ± 159.2 nm were formed. From the HR-TEM image of 15% Ag/Ag3PO4/BiPO4, the resolved lattice spacing was determined to be 0.131 and 0.249 nm, which is consistent with the d spacing of the (421) plane of the body-centered cubic phase of Ag3PO4 and the (11) plane of the monoclinic phase of BiPO4, respectively. Finally, adding 30% Ag+ to BiPO4 resulted in shorter rod-like Ag/Ag3PO4/BiPO4 structures with diameters of 182.8 ± 54.2 nm and lengths of 853.8 ± 79.2 nm. The HR-TEM image of 30% Ag/Ag3PO4/BiPO4 indicated the existence of a distinct lattice spacing of 0.465 nm, which corresponds to the (011) crystal plane of BiPO4.
The BET specific surface areas of the BiPO4 and X% Ag/Ag3PO4/BiPO4 samples (X = 3, 6, 15, and 30) were also determined using nitrogen adsorption–desorption measurements and the corresponding values are listed in Table 1. As shown in Table 1, the BET surface areas values increases with increasing the amount of Ag+. Therefore, BiPO4 with Ag+ impregnation is expected to have higher adsorption capacity and photocatalytic activity for the degradation of dye in water.
Series | Pseudo first-order kinetic equation | R2 | Surface area (m2 g−1) |
---|---|---|---|
BiPO4 | y = 0.0347x − 0.0306 | 0.9720 | 3.5 ± 0.1 |
3% Ag/Ag3PO4/BiPO4 | y = 0.0538x − 0.0538 | 0.9977 | 30.1 ± 0.1 |
6% Ag/Ag3PO4/BiPO4 | y = 0.1021x − 0.0609 | 0.9903 | 42.5 ± 0.3 |
15% Ag/Ag3PO4/BiPO4 | y = 0.2593x − 0.1372 | 0.9919 | 55.1 ± 0.1 |
30% Ag/Ag3PO4/BiPO4 | y = 0.2546x − 0.1072 | 0.9892 | 70.1 ± 0.1 |
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Fig. 3 (a) Photocatalytic decomposition curves for MB and (b) kinetic fit for MB degradation catalyzed by BiPO4 and Ag/Ag3PO4/BiPO4. |
Fig. S4(a) and (b)† show the temporal evolution of the spectral change upon MB degradation over BiPO4 and 15% Ag/Ag3PO4/BiPO4, respectively. According to literature, chromophore cleavage is analogous to a competitive photodegradation reaction involved in the photocatalytic decomposition of organic pollutants.26 The absorption of MB at 665 nm decreased with an increase in the irradiation time. Moreover, the characteristic absorption of MB in the presence of BiPO4 and 15% Ag/Ag3PO4/BiPO4 decreased only insignificantly and exhibited a slight hypsochromic shift. Thus, the cleavage of the MB chromophore is inferred to predominate in both BiPO4 and 15% Ag/Ag3PO4/BiPO4 photocatalytic decomposition systems.
To further investigate the photocalalytic activity of the various photocatalysts (P25, BiPO4, Ag/Ag3PO4, and 15% Ag/Ag3PO4/BiPO4), RhB, MO, and MB degradation under solar irradiation was analyzed; the results are shown in Fig. 4(a). 15% Ag/Ag3PO4/BiPO4 exhibited excellent photocatalytic activity than that of the P25 and BiPO4 photocatalyst under solar irradiation for the degradation of all dyestuffs, with nearly 100% degradation achieved in only 5 min. This may be because of absorption in the visible region of sunlight. In addition, we found 15% Ag/Ag3PO4/BiPO4 could also be easily recovered by sedimentation due to high density of Ag3PO4 (6.37 g cm−3) comparing to BiPO4 (6.32 g cm−3) and TiO2 (4.23 g cm−3), which is beneficial for the applications in water purification. Although the Ag/Ag3PO4 also exhibited the similar photocatalytic activity to that of the 15% Ag/Ag3PO4/BiPO4 due to high absorption in the visible region of sunlight, the amount of AgNO3 for the preparation of the Ag/Ag3PO4 (0.21 g) is more than that of the 15% Ag/Ag3PO4/BiPO4 (0.045 g) photocatalyst. This 15% Ag/AgP3O4/BiPO4 photocatalyst possesses attractive features (low cost) when compared with Ag/Ag3PO4 heterostructures. According to literatures, long UV irradiation also effectively induces electron–hole separation in the BiPO4.4,10,12 This can further improve the photocalytic activity of 15% Ag/Ag3PO4/BiPO4 for the practical applications.
To further test the practicality of 15% Ag/Ag3PO4/BiPO4, the photocatalytic performance was evaluated for MB degradation in environmental water samples under solar irradiation. Fig. 4(b) presents variations in the MB concentration (C/C0) with the time of irradiation over 15% Ag/Ag3PO4/BiPO4, where C0 is the initial MB concentration and C is the MB concentration at time t. For all of the environmental water samples, in the presence of 15% Ag/Ag3PO4/BiPO4, the MB concentration decreased with an increase in the reaction time, indicating that the as-prepared material is an active photocatalyst. A remarkable difference in MB degradation with time was observed for the pond water (within 5 min) than that for the seawater and industrial wastewater (within 20 min). This may be because anions or radical scavengers in the seawater and industrial wastewater samples reduced the photocatalytic activity of 15% Ag/Ag3PO4/BiPO4. Further research on the high photocatalytic activity of other heterojunction BiPO4 composites, such as those enwrapped by graphene oxide and carbon nanotubes, is now underway in our laboratory.27–31
Next, to test the microorganism disinfection ability, the photocatalytic disinfection of 15% Ag/Ag3PO4/BiPO4 was evaluated using the model waterborne pathogen E. coli. Fig. 5(a) presents plots of the variation in the E. coli colony forming units (n/n0) with the irradiation time for the control and 15% Ag/Ag3PO4/BiPO4, where n0 is the initial E. coli colony forming units, and n is the E. coli colony forming units at time t. It shows that 90% E. coli removal occurred in the presence of 15% Ag/Ag3PO4/BiPO4 under sunlight irradiation for 30 min. The bactericidal activity of the sample is also confirmed by the images of colonies incubated on an agar plate the control and 15% Ag/Ag3PO4/BiPO4 under sunlight irradiation (image d and e in the Fig. 5). Interesting, 15% Ag/Ag3PO4/BiPO4 also presents the intrinsic antibacterial activity in the dark condition for 30 min (about 40% E. coli cell removal, shown in the Fig. 5(a), image b and c in the Fig. 5). As we known, Ag-based composites are to be effective biocides against many bacteria.31 Thus, it is reasonable to suggest that the Ag/Ag3PO4/BiPO4 could be used for the disinfection applications.
First, the photocurrent responses of BiPO4 and 15% Ag/Ag3PO4/BiPO4 were measured to reflect the separation efficiency of the photogenerated electrons and holes. Uniform photocurrent responses to the light were detected (Fig. S6(a)†). In addition, the photocurrent response of 15% Ag/Ag3PO4/BiPO4 was higher than that of BiPO4 (three times), indicating enhanced separation of photogenerated electrons and holes. Moreover, a heterostructure was formed between Ag and Ag3PO4 nanoparticles. Such heterostructures can also improve the separation of photogenerated electrons and holes through the Schottky barrier effect, which is consistent with a previous study on electron transfer from a semiconductor to a metal.20 Ag nanoparticles on the Ag3PO4 surface act as absorbents for electrons; this contributes to the interfacial charge transfer between the metal and semiconductor and to the separation of photogenerated electrons and holes, thus enhancing the photocatalytic activity.
The recombination of electron–hole pairs can release energy in the form of PL emission. A low electron–hole recombination rate implies a lower luminescence emission intensity and higher photocatalytic activity.9 Thus, to understand the recombination rates of the electron–hole pairs during photocatalysis using BiPO4 and 15% Ag/Ag3PO4/BiPO4, the PL emission spectra of the samples were measured at λex = 250 nm (Fig. S6(b)†). The emission intensity of BiPO4 was greater than that of 15% Ag/Ag3PO4/BiPO4, indicating that the electron–hole pairs in BiPO4 recombine rapidly. As mentioned earlier, the heterostructure interface between the BiPO4 and Ag3PO4 nanoparticles had numerous defects that suppressed the recombination of photogenerated electrons and holes, resulting in increased photocatalytic activity.
Radical- and hole-trapping experiments were designed to elucidate the photocatalytic degradation process for 15% Ag/Ag3PO4/BiPO4. Under irradiation, MB photodegradation was suppressed upon the addition of the hole scavenger disodium ethylenediamine tetraacetate (EDTA-2Na) but only slightly inhibited upon the addition of the radical scavenger tert-butyl alcohol (Fig. S7(a)†). These results indicate that a hole is the primary active species involved in the decomposition of the adsorbed organic pollutants. Therefore, holes play a crucial role in the Ag/Ag3PO4/BiPO4 photocatalytic system. Hydroxyl radicals can be formed through the hole oxidation of OH− or the reduction of O2. The former route is controlled by the potential of the holes in the valence band.32,33 The effect of using a N2 atmosphere is shown in Fig. S7(b).† In an anoxic suspension, MB photodegradation decreased, which indicated that O2 is also an essential source for the generation of superoxide species and hydroxyl radicals via photoreduction. To further confirm the existence of hydroxyl radicals, BiPO4 and 15% Ag/Ag3PO4/BiPO4 illuminated by Xe light were examined using the PL technique. The PL emission spectra, excited at 370 nm in the coumarin solution containing a suspension of BiPO4 or 15% Ag/Ag3PO4/BiPO4, were measured after each sample was illuminated for 15 min. Fig. S8† shows that a PL signal was observed at 516 nm for each sample. The maximum PL intensity was observed for 15% Ag/Ag3PO4/BiPO4. This suggests that the fluorescence was due to chemical reactions of coumarin with hydroxyl radicals formed in the photocatalytic reactions.22 Hence, the hydroxyl radical is the indirect reactive oxidation species in the Ag/Ag3PO4/BiPO4 samples and finally induces MB degradation.
On the basis of the aforementioned discussion, a possible mechanism for the increased photodegradation activity and stability of the Ag/Ag3PO4/BiPO4 heterostructures is presented in Scheme 1. The conduction band (CB) and valence band (VB) positions in BiPO4 and Ag/Ag3PO4 were calculated using the equation EVB = X − Ee + 0.5 Eg, where X is the Mulliken electronegativity (XAg3PO4: 5.961 eV, XBiPO4: 6.492 eV), Ee is the energy of free electrons on the hydrogen scale (≅4.5 eV), and Eg is the bandgap. The EVB for the BiPO4 and Ag3PO4 were thus estimated to be 4.032 and 2.486 eV, meanwhile the ECB of them were −0.048 and 0.436 eV, respectively. The illumination energy of sunlight can be efficiently absorbed by Ag/Ag3PO4/BiPO4. The electron in the VB can be excited to the CB with simultaneous generation of the same amount of holes in the VB. Because the energy position of the CB of the Ag3PO4 is lower than that of the BiPO4, Ag/Ag3PO4/BiPO4 heterostructures would produce an interface. Therefore, the generated electrons in CB are limited to immigrate from BiPO4 (electronic barrier) to Ag3PO4 (electronic potential well). The generated electron from Ag3PO4 and BiPO4 can be quickly reacted with water and oxygen for the generation of superoxide species. However, superoxide specie is not the primary active species in the decomposition of the adsorbed organic pollutants. The energy level of the VB of the Ag3PO4 is higher than that of the BiPO4; the generated holes in VB are thus immigrated from BiPO4 to Ag3PO4 in the Ag/Ag3PO4/BiPO4 heterostructures, whereas the accumulated holes on Ag3PO4 to oxidize organic substances. Therefore, Ag/Ag3PO4/BiPO4 suppresses the recombination of electron–hole pairs because of the heterostructure interface. In addition, Ag nanoparticles on the Ag3PO4 surface also act as electron acceptors, thus contributing to the separation of photogenerated electron–hole pairs. These two factors enhance the production of active holes and hydroxyl radicals, which decompose MB. Furthermore, excess electrons favor the presence of Ag nanoparticles that also decrease the reduction of Ag+ of the Ag3PO4 photocatalyst, thus increasing the stability of the photocatalyst.20,24
This novel Ag/AgP3O4/BiPO4 photocatalyst possesses several attractive features when compared with different Ag/Ag3PO4/BiPO4-based heterostructures (Table 2): (1) facile and simplicity—sophisticated preparation process is not required; (2) high stability and photocatalytic performance—95% photocatalytic degradation of various organic dyes (MB, RhB, and MO) is observed within 5 min; (3) practicality—the sunlight induced photocatalytic degradation of dyes in the complicated samples (seawater, pond water, and industrial wastewater samples) and disinfection of E. coli cells are possible. Further application research using this novel Ag/AgP3O4/BiPO4 photocatalyst, such as water purification and direct methanol fuel cells, is now underway in our laboratory.
Photocatalyst | Synthesis method | Photocatalytic activity (λ > 420 nm) | Sunlight irradiation | Stability | Degradation target | Environmental water samples | Ref. |
---|---|---|---|---|---|---|---|
a Not provided.b Mercury lamp with main emission wavelength 313 nm. | |||||||
BiPO4@Ag3PO4 | Hydrothermal process and ion-exchange method | 95% degradation (0.05 g photocatalyst/20 ppm RhB) within 60 min (500 W) | 95% degradation (0.05 g photocatalyst/20 ppm RhB) within 40 min | —a | RhB | —a | 19 |
Ag/Ag3PO4/BiPO4 | Low temperature chemical bath method | 98% degradation (0.1 g photocatalyst/10 ppm RhB) within 60 min (300 W) | —a | —a | RhB | —a | 20 |
Ag3PO4/BiPO4 | Co-precipitation hydrothermal method | 97% degradation (0.1 g photocatalyst/10 ppm MO) within 30 min (500 W) | —a | 3 recycling | MO | —a | 21 |
BiPO4/Ag | Sonochemical synthesis | 100% degradation (0.03 g photocatalyst/9.6 ppm RhB) within 120 min (150 W) | —a | 5 recycling | RhB | —a | 25 |
Ag/BiPO4 | Hydrothermal and impregnation processes | 90% degradation (0.05 g photocatalyst/3.2 ppm MB) within 20 min (500 W)b | —a | 5 recycling | MB | —a | 26 |
Ag/Ag3PO4/BiPO4 | Hydrothermal and impregnation processes | 95% degradation (0.2 g photocatalyst/5 ppm MB) within 15 min (150 W) | 95% degradation (0.2 g photocatalyst/5 ppm MB) within 5 min | 5 recycling | MB, RhB, MO, E. coli cell | Seawater, pond water, industrial wastewater samples | This study |
Footnote |
† Electronic supplementary information (ESI) available: Fig. S1. Molecular structures of MB, RhB, and MO. Fig. S2. (a) Raman and (b) FTIR spectra of as-prepared BiPO4, Ag/Ag3PO4/BiPO4, and Ag/Ag3PO4. Fig. S3. XPS spectra of as-prepared Ag/Ag3PO4/BiPO4. Fig. S4. Temporal evolution of the spectral change upon MB degradation over (a) BiPO4 and (b) 15% Ag/Ag3PO4/BiPO4. Fig. S5. (a) Cycling runs of MB photocatalytic degradation in the presence of 15% Ag/Ag3PO4/BiPO4 products and (b) XRD pattern for 15% Ag/Ag3PO4/BiPO4 after being used for five reaction cycles. Fig. S6. (a) Photocurrents and (b) PL spectra measured at λex = 250 nm of BiPO4 and 15% Ag/Ag3PO4/BiPO4. Fig. S7. (a) Plots of photogenerated carrier trapping for MB photodegradation catalyzed by 15% Ag/Ag3PO4/BiPO4. (b) Effect of O2 and N2 on MB photocatalytic degradation in the presence of 15% Ag/Ag3PO4/BiPO4. Fig. S8. PL spectra of BiPO4 and 15% Ag/Ag3PO4/BiPO4 in coumarin solution measured at λex = 370 nm (each sample was illuminated for 15 min under visible light). See DOI: 10.1039/c5ra07101a |
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